“…Eq. (39), into the prescription H j,j+n = (1 2)Ψ † H j,j+n Ψ, we find that only four of them, corresponding to (a), (b), (g), and (h), give a nonzero second-quantized Hamiltonian. In the other four cases, the hermiticity of H j,j+n when combined with the fermion algebra cancels out the resulting second-quantized expressions, signaling an incompatibility with fermion statistics.…”